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Baryon self-energy due to the pion-quark interaction

Journal Article · · Phys. Rev. D; (United States)
We examine the baryon self-energy due to the pion-quark interaction, more specifically, how the self-energy varies among the ground states of the baryon octet and decuplet, and also from the ground to excited states. A nonrelativistic constituent quark model is used in which quarks are bound in a harmonic-oscillator potential. For the excited states we examine the lowest even- and odd-parity states in the nucleon sector. We find that the variation of the self-energy within the same strangeness sector is quite small, i.e., of the order of 30 MeV or smaller. For example, the pion contribution to the ..delta..-N splitting is < or approx. =20 MeV. In arriving at this small variation it is crucial to take account of the spin dependence of the quark energy that enters in the energy denominator of the self-energy calculation. The individual energy shift is sensitive to the (ad hoc) form factor associated with the pion-quark interaction, and also to the quark excitation in the intermediate state. However, this sensitivity is strongly reduced in the difference between energy shifts for different baryon states.
Research Organization:
Department of Physics, McMaster University, Hamilton, Ontario, Canada L8S 4M1
OSTI ID:
5008148
Journal Information:
Phys. Rev. D; (United States), Journal Name: Phys. Rev. D; (United States) Vol. 32:11; ISSN PRVDA
Country of Publication:
United States
Language:
English